Final Magnetic Moment0.002 μBCalculated total magnetic moment for the unit cell within the magnetic ordering provided (see below). Typically accurate to the second digit. |
Magnetic OrderingNM |
Formation Energy / Atom0.619 eVCalculated formation energy from the elements normalized to per atom in the unit cell. |
Energy Above Hull / Atom0.799 eVThe energy of decomposition of this material into the set of most stable materials at this chemical composition, in eV/atom. Stability is tested against all potential chemical combinations that result in the material's composition. For example, a Co2O3 structure would be tested for decomposition against other Co2O3 structures, against Co and O2 mixtures, and against CoO and O2 mixtures. |
Density5.97 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToGe + BeTe |
Band Gap0.000 eVIn general, band gaps computed with common exchange-correlation functionals such as the LDA and GGA are severely underestimated. Typically the disagreement is reported to be ~50% in the literature. Some internal testing by the Materials Project supports these statements; typically, we find that band gaps are underestimated by ~40%. We additionally find that several known insulators are predicted to be metallic. |
Hermann MauguinF43m [216] |
HallF 4 2 3 |
Point Group43m |
Crystal Systemcubic |
Calculated powder diffraction pattern; note that peak spacings may be affected due to inaccuracies in calculated cell volume, which is typically overestimated on average by 3% (+/- 6%)
Select an element to display a spectrum averaged over all sites of that element in the structure.
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Download spectra for every symmetrically equivalent absorption site in the structure.
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substrate material | substrate orientation | film orientation | MCIA† [Å2] |
---|---|---|---|
AlN (mp-661) | <0 0 1> | <1 0 0> | 230.8 |
AlN (mp-661) | <1 0 1> | <1 0 0> | 323.2 |
CeO2 (mp-20194) | <1 1 0> | <1 1 0> | 130.6 |
GaAs (mp-2534) | <1 1 1> | <1 1 1> | 239.9 |
SiO2 (mp-6930) | <1 0 0> | <1 1 0> | 326.5 |
LaAlO3 (mp-2920) | <0 0 1> | <1 0 0> | 230.8 |
LaAlO3 (mp-2920) | <1 1 0> | <1 1 0> | 130.6 |
AlN (mp-661) | <1 1 0> | <1 1 0> | 326.5 |
CeO2 (mp-20194) | <1 0 0> | <1 0 0> | 230.8 |
CeO2 (mp-20194) | <1 1 1> | <1 1 0> | 261.2 |
GaAs (mp-2534) | <1 1 0> | <1 1 0> | 195.9 |
DyScO3 (mp-31120) | <1 0 1> | <1 0 0> | 277.0 |
InAs (mp-20305) | <1 0 0> | <1 0 0> | 184.7 |
ZnSe (mp-1190) | <1 1 1> | <1 1 1> | 239.9 |
CdS (mp-672) | <0 0 1> | <1 1 1> | 319.9 |
GaN (mp-804) | <0 0 1> | <1 1 1> | 80.0 |
GaN (mp-804) | <1 1 0> | <1 1 0> | 261.2 |
DyScO3 (mp-31120) | <0 1 1> | <1 1 1> | 159.9 |
LiF (mp-1138) | <1 1 0> | <1 1 0> | 261.2 |
Te2W (mp-22693) | <0 1 0> | <1 0 0> | 323.2 |
ZnSe (mp-1190) | <1 1 0> | <1 1 0> | 195.9 |
KTaO3 (mp-3614) | <1 1 1> | <1 0 0> | 138.5 |
CdS (mp-672) | <1 0 0> | <1 1 0> | 195.9 |
CdS (mp-672) | <1 1 0> | <1 1 0> | 195.9 |
Te2W (mp-22693) | <0 1 1> | <1 0 0> | 230.8 |
Ag (mp-124) | <1 0 0> | <1 0 0> | 230.8 |
Ag (mp-124) | <1 1 0> | <1 1 0> | 195.9 |
Bi2Te3 (mp-34202) | <0 0 1> | <1 1 0> | 261.2 |
GaSe (mp-1943) | <0 0 1> | <1 0 0> | 230.8 |
BN (mp-984) | <0 0 1> | <1 0 0> | 230.8 |
Bi2Se3 (mp-541837) | <0 0 1> | <1 1 1> | 239.9 |
MoS2 (mp-1434) | <0 0 1> | <1 1 1> | 80.0 |
Al (mp-134) | <1 1 0> | <1 1 0> | 261.2 |
CdTe (mp-406) | <1 1 1> | <1 1 1> | 80.0 |
C (mp-66) | <1 0 0> | <1 0 0> | 230.8 |
C (mp-66) | <1 1 0> | <1 1 0> | 195.9 |
LaF3 (mp-905) | <0 0 1> | <1 1 1> | 319.9 |
PbS (mp-21276) | <1 0 0> | <1 0 0> | 184.7 |
PbS (mp-21276) | <1 1 0> | <1 1 0> | 195.9 |
GaP (mp-2490) | <1 1 0> | <1 1 0> | 130.6 |
GaP (mp-2490) | <1 1 1> | <1 1 0> | 261.2 |
InP (mp-20351) | <1 0 0> | <1 0 0> | 184.7 |
Ni (mp-23) | <1 1 0> | <1 1 0> | 195.9 |
InSb (mp-20012) | <1 0 0> | <1 0 0> | 46.2 |
InSb (mp-20012) | <1 1 0> | <1 1 0> | 65.3 |
NdGaO3 (mp-3196) | <0 1 0> | <1 1 0> | 130.6 |
NdGaO3 (mp-3196) | <1 0 1> | <1 1 1> | 159.9 |
SiC (mp-11714) | <1 0 1> | <1 0 0> | 323.2 |
MoSe2 (mp-1634) | <0 0 1> | <1 0 0> | 230.8 |
Ga2O3 (mp-886) | <1 0 -1> | <1 0 0> | 184.7 |
A full elastic tensor has not been calculated for this material. Registered users can view statistical-learning-based predictions of this material's bulk and shear moduli.
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material | dissimilarity | Ehull | # of elements |
---|---|---|---|
TmAlAg2 (mp-980426) | 0.0000 | 0.000 | 3 |
Pr2HgPb (mp-861498) | 0.0000 | 0.006 | 3 |
ThCdRh2 (mp-861646) | 0.0000 | 0.001 | 3 |
Sr2LiTl (mp-862746) | 0.0000 | 0.000 | 3 |
LiSnAu2 (mp-865710) | 0.0000 | 0.000 | 3 |
TiFeCoAs (mp-998974) | 0.0000 | 0.134 | 4 |
TiGaFeCo (mp-998964) | 0.0000 | 0.000 | 4 |
TiFeCoSb (mp-998973) | 0.0000 | 0.186 | 4 |
TiAlFeCo (mp-998980) | 0.0000 | 0.000 | 4 |
MnGaFeCo (mp-999552) | 0.0000 | 0.044 | 4 |
Yb3In (mp-980052) | 0.0000 | 0.069 | 2 |
HoTa3 (mp-973969) | 0.0000 | 0.380 | 2 |
LaAu3 (mp-976113) | 0.0000 | 0.037 | 2 |
Na3N (mp-999495) | 0.0000 | 0.506 | 2 |
Nb3Fe (mp-999395) | 0.0000 | 0.085 | 2 |
Cu (mp-998890) | 0.0000 | 0.037 | 1 |
Kr (mp-974400) | 0.0000 | 0.002 | 1 |
H2 (mp-632250) | 0.0000 | 0.000 | 1 |
Ge (mp-998883) | 0.0000 | 0.339 | 1 |
U (mp-108) | 0.0000 | 0.269 | 1 |
Run TypeGGA |
Energy Cutoff520 eV |
# of K-pointsNone |
U Values-- |
PseudopotentialsVASP PAW: Be_sv Ge_d Te |
Final Energy/Atom-3.4127 eV |
Corrected Energy-13.6509 eV
-13.6509 eV = -13.6509 eV (uncorrected energy)
|
Displaying lattice parameters for primitive cell; note that calculated cell volumes are typically overestimated on average by 3% (+/- 6%). Note the primitive cell may appear less symmetric than the conventional cell representation (see "Structure Type" selector below the 3d structure)